dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2013-09-30T18:53:41Z
dc.date.accessioned2014-05-20T14:09:32Z
dc.date.accessioned2022-10-05T15:05:19Z
dc.date.available2013-09-30T18:53:41Z
dc.date.available2014-05-20T14:09:32Z
dc.date.available2022-10-05T15:05:19Z
dc.date.created2013-09-30T18:53:41Z
dc.date.created2014-05-20T14:09:32Z
dc.date.issued2010-04-01
dc.identifierJournal of High Energy Physics. New York: Springer, n. 4, p. 13, 2010.
dc.identifier1126-6708
dc.identifierhttp://hdl.handle.net/11449/24184
dc.identifier10.1007/JHEP04(2010)067
dc.identifierWOS:000277473100003
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/3897381
dc.description.abstractFour-dimensional super-twistors provide a compact covariant description of on-shell N = 4 d=4 super-Yang-Mills. In this paper, ten-dimensional super-twistors are introduced which similarly provide a compact covariant description of on-shell d=10 super-Yang-Mills. The super-twistor variables are Z - (lambda(alpha), mu(alpha), Gamma(m)) where lambda(alpha) and mu(alpha) are constrained bosonic d=10 spinors and Gamma(m) is a constrained fermionic d=10 vector. The Penrose map relates the twistor superfield Phi(Z) with the d=10 super-Yang-Mills vertex operator lambda(alpha) A(alpha)(x,theta) which appears in the pure spinor formalism of the superstring, and the cubic super-Yang-Mills amplitude is proportional to the super- twistor integral f dZ Phi(1)Phi(2)Phi(3).
dc.languageeng
dc.publisherSpringer
dc.relationJournal of High Energy Physics
dc.relation1,227
dc.rightsAcesso restrito
dc.sourceWeb of Science
dc.subjectSuperspaces
dc.subjectField Theories in Higher Dimensions
dc.titleTen-dimensional super-twistors and Super-Yang-Mills
dc.typeArtigo


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